The transparency of the Universe to Very High Energy photons - - PowerPoint PPT Presentation

the transparency of the universe to very high energy
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The transparency of the Universe to Very High Energy photons - - PowerPoint PPT Presentation

The transparency of the Universe to Very High Energy photons Barbara De Lotto - University of Udine & INFN Outline: Photon propagation Observations of distant AGN Physics interpretation Conclusions Vulcano Workshop 2010


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The transparency of the Universe to Very High Energy photons

Vulcano Workshop 2010 – Frontier Objects in Astrophysics and Particle Physics – May 2010

Outline:

  • Photon propagation
  • Observations of distant AGN
  • Physics interpretation
  • Conclusions

Barbara De Lotto - University of Udine & INFN

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VHE γ-rays have opened a new window on the Universe

2010

GRBs AGN Pulsars PWN μ μ-

  • quasar

quasar SNRs

  • rigin of

cosmic rays

cosmology cosmology

dark matter

space time

Scientific targets

Spectral characteristics

  • f blazars

Cosmic background radiation

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Intergalactic absorption of VHE photons

Around the TeV region cross section maximized for infrared/optical photons (Extragalactic Background Light)

(Heitler 1960)

maximal for ε :

( )

θ ε β cos 1 2 1

4 2

− − = E c me

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Extragalactic Background Light

  • Thermal emission produced by stars

and partly absorbed/re-emitted by dust during the entire history of the Universe

  • two components
  • Several models try to describe the

EBL Spectral Energy Distribution: main differences depending on how the evolution in time and frequency is treated n(ε,z)

Finke & Razzaque arXiv0905.1115v2

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Attenuation

nε (ε,z) spectral energy density of background photons (EBL)

) , ( em

  • bs

) ( ) , (

z E

e E z E

τ −

× Φ ≡ Φ

τ

  • ptical depth
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(An approximation)

  • Neglecting evolutionary

effects for simplicity

Coppi & Aharonian ApJ 1997

τ(E,D) ≈ D Λ(E) Λ ∝ 1 σ ⎛ ⎝ ⎜ ⎞ ⎠ ⎟ Φobs(E,D) ≈ Φem(E) × e

− D Λ(E )

For γ-rays energies above a few TeV, the distance they can propagate ≤ 100 Mpc most of the VHE Universe seems not visible to us

Λ (Mpc)

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Consequences

  • Since Λ

becomes < RHubble for E > 100 GeV:

– The observed flux should be exponentially suppressed at VHE the observed spectrum should be steeper than the emitted one. – The observed flux should be exponentially suppressed at large distances very far-away sources should become invisible as energy increases

γ – ray horizon: τ(E,z) = 1

Fazio & Stecker 1970

~ E-2

τ = 1

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The far away VHE Universe …

38 Sources …

PKS 0447-439 z=0.20 HESS 2009 1ES 1011+496 z=0.21 MAGIC 2007 1ES 0414+009 z=0.29 HESS & Fermi 2009 S5 0716+71 z=0.31±0.08 MAGIC 2009 1ES 0502+675 z=0.34 VERITAS 2009 3C 66A z=0.44 VERITAS 2009 3C 279 z=0.54 MAGIC 2008

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The distant quasar 3C 279

  • Flat spectrum radio quasar at z = 0.54
  • Very bright and strongly variable

– Brightest EGRET AGN – Gamma-ray flares in 1991 and 1996. Fast time variation (~ 6hr in 1996 flare)

  • MAGIC observations

– 10 h between Jan.-April 2006 – clear detection on 23rd Feb. at 6.2σ First FSRQ in TeV γ-rays Major jump in redshift Science 320 (2008) 1752

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Follow up observations of 3C 279

  • New observations after optical outburst in Jan. 2007

new flare detected

Most distant object ever detected at VHE - two flares

(Feb. 2006 and Jan. 2007) Hard spectrum confirmed

  • E. Carmona – HEAD2010
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Implications on Extragalactic Background Light

e-

γVHE

  • Power law Γ

= 4.1 ± 0.7, measured up to 0.5 TeV Spectrum sensitive to 0.2 - 2 μm

  • Assume minimum reasonable index Γem

= 1.5 Upper limit close to lower limit from galaxy count Emission harder than expected

Universe more transparent

to γ-rays than expected The measurement of spectral features permits to constrain EBL models:

Γ

e+ γEBL blazar IACT e-

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  • At ~ 0.5 TeV, flux attenuated by 2
  • rders of magnitude

even for the lowest EBL model:

  • Possible explanations:

– from standard ones

  • very hard emission mechanisms with intrinsic slope < 1.5 (Stecker 2008)
  • Very low EBL

– to possible evidence for new physics …

Could it be seen?

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Is there a new land just behind the horizon?

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Oscillation to an Axion-Like Particle

( )a

B E M

a

⋅ = 1

γ

L

  • available constraints in the parameters m, M:

CAST exp. & astrophysical arguments: M > 1010 GeV, m < 0.01 eV (PDG 08)

  • Intergalactic magnetic field:

domain-like structure with strength ~ 0.5 nG, coherence length λ ~ 10 Mpc, random orientation in each domain RESULTS: Small mass , small coupling (within limits) naturally explain the enhancement at large E

during the propagation in the

intergalactic medium [DeAngelis,Roncadelli& Mansutti, PLB2008, PRD2008]:

m <<10−10eV (maximal mixing) 1011 GeV < M < 1013 GeV

in the presence of magnetic fields. Several interpretations:

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SLIDE 15

… continue

Simet, Hooper & Serpico, PRD 08

  • Conversion at the emission
  • Milky Way acts as a converter to

photons

Sanchez-Conde et al., PRD 09

  • Mixing inside the source and in the

intergalactic magnetic field simultaneously considered in the same framework

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Experimental input from more sources at high z:

MAGIC S5 0716+714

  • MAGIC discovery 23rd – 25th April, Atel 29th
  • On 28th Swift reports high flux (0.3-10 KeV)
  • MAGIC flux(>400 GeV) ≈25% Crab,

Γ = 3.45±0.54

  • 3rd low-peaked VHE blazar after BL Lac & W

comae

  • Host galaxy detected: z = 0.31±0.08 => 3rd

farthest VHE emitter for which the spectral index has been measured Optical light curve: KVA telescope, La Palma

ApJ 704 (2009) L129

  • 3rd MAGIC discovery after optical ToO
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Spectral characterstics of observed AGN: a synoptic view

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PKS 0447-439 z=0.20 HESS 2009 1ES 1011+496 z=0.21 MAGIC 2007 1ES 0414+009 z=0.29 HESS & Fermi 2009 S5 0716+71 z=0.31±0.08 MAGIC 2009 1ES 0502+675 z=0.34 VERITAS 2009 3C 66A z=0.44 VERITAS 2009 3C 279 z=0.54 MAGIC 2008

…and more new sources are coming into the game (VERITAS, HESS, MAGIC) spectral index redshift z

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Where do we stand ?

  • Recent gamma observations might present substantial challenges to the

conventional models to explain the observed source spectra and/or EBL density. – MAGIC 3C279 at z=0.54; VERITAS detection above 0.1 TeV from 3C66A (z=0.44): EBL-corrected spectrum harder than 1.5 (Acciari+, ApJ09);

  • TeV photons coming from 3C 66A? (Neshpor+98; Stepanyan+02). Difficult to explain with

conventional EBL and physics.

– The lower limit on the EBL at 3.6 μm was recently revised upwards by a factor ∼2, suggesting a more opaque Universe (Levenson+08). Some sources at z = 0.1 − 0.2 seem to have harder intrinsic energy spectra than previously anticipated (Krennrich+08). – Spectral indices don’t grow with increasing distance: selection bias?

  • While it is still possible to explain the above points with conventional physics,

the axion/photon oscillation could naturally explain these puzzles

18

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Other possible explanations related to new physics

  • Kifune 2001: Violation of the Lorentz

invariance “a la Coleman-Glashow”:

the absorption mean free path of VHE γ – rays is altered by orders of magnitude from those conventionally estimated.

c2p2 = E2 1+ξ E Es +O E Es ⎛ ⎝ ⎜ ⎞ ⎠ ⎟

2

⎡ ⎣ ⎢ ⎢ ⎤ ⎦ ⎥ ⎥

but

we should keep in mind that

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Conclusions

  • VHE γ

–rays have opened a new window in the Universe

  • The observation of VHE γ

–rays from extragalactic sources (like blazars) has entered a new era, thanks to the new generation

  • f ground based Cherenkov telescopes (and Fermi)
  • To disentangle attenuation due to EBL from intrinsic properties
  • f blazars, and eventually probe certain aspects of fundamental

new physics, the detection of more sources at different redshifts is essential

  • We have the tool: increased sensitivity of the upgraded current

telescopes (like MAGIC) in synergy with Fermi, and possibly a future Cherenkov Telescope Array system (CTA project).

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”A textbook example of the merging of particle physics and astronomy into the modern field of astroparticle physics”

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BACKUP

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Imaging Air Cherenkov Technique Imaging Air Cherenkov Technique

~ 10 km Particle shower

~ 1o

Cherenkov light

~ 120 m

Gamma ray Cherenkov light Image of particle shower in telescope camera

  • reconstruct:

arrival direction, energy

  • reject hadron background

statistically in the analysis

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  • Axions were postulated to solve the strong CP problem in the 70s.
  • Good Dark Matter candidates (axions with masses ≈

meV-μeV could account for the total Dark Matter content).

  • They are expected to oscillate into photons (and viceversa) in the presence of

magnetic fields: Photon/axion oscillations are the main vehicle used at present in axion searches (ADMX, CAST…). Some astrophysical environments fulfill the mixing requirements AGNs, IGMFs M11 : coupling constant inverse (gαγ /1011 GeV) BG : magnetic field (G) spc : size region (pc) with

15⋅ BG ⋅ spc M11 ≥1